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9789810247195

Nonadiabatic Transitions : Concepts, Basic Theories and Applications

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  • ISBN13:

    9789810247195

  • ISBN10:

    9810247192

  • Format: Hardcover
  • Copyright: 2002-08-01
  • Publisher: WORLD SCIENTIFIC PUB CO INC
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Summary

Nonadiabatic transition is a highly multidisciplinary concept and phenomenon, constituting a fundamental mechanism of state and phase changes in various dynamical processes of physics, chemistry and biology, such as molecular dynamics, energy relaxation, chemical reaction, and electron and proton transfer.

Table of Contents

Preface v
Introduction: What is ``Nonadiabatic Transition''?
1(6)
Multi-Disciplinarity
7(12)
Physics
7(6)
Chemistry
13(3)
Biology
16(1)
Economics
16(3)
Historical Survey of Theoretical Studies
19(22)
Landau-Zener-Stueckelberg Theory
19(9)
Rosen-Zener-Demkov Theory
28(3)
Nikitin's Exponential Model
31(2)
Nonadiabatic Transition Due to Coriolis Coupling and Dynamical State Representation
33(8)
Background Mathematics
41(12)
Wentzel-Kramers-Brillouin Semiclassical Theory
41(4)
Stokes Phenomenon
45(8)
Basic Two-State Theory for Time-Independent Processes
53(68)
Exact Solutions of the Linear Curve Crossing Problems
53(12)
Landau-Zener type
53(9)
Nonadiabatic tunneling type
62(3)
Complete Semiclassical Solutions of General Curve Crossing Problems
65(24)
Landau-Zener (LZ) type
66(5)
E ≥ Ex (b2 ≥ 0)
71(2)
E ≤ Ex (b2 ≤ 0)
73(1)
Numerical examples
74(4)
Nonadiabatic Tunneling (NT) Type
78(3)
E ≤ Et (b2 ≤ -1)
81(1)
Et ≤ E ≤ Eb (|b2| ≤ 1)
82(1)
E ≥ Eb (b2 ≥ 1)
83(1)
Complete reflection
84(1)
Numerical examples
85(4)
Non-Curve-Crossing Case
89(4)
Rosen-Zener-Demkov model
89(1)
Diabatically avoided crossing model
90(3)
Exponential Potential Model
93(15)
Mathematical Implications
108(13)
Case (i)
112(3)
Case (ii)
115(3)
Case (iii)
118(3)
Basic Two-State Theory for Time-Dependent Processes
121(24)
Exact Solution of Quadratic Potential Problem
121(5)
Semiclassical Solution in General Case
126(9)
Two-crossing case: β ≥ 0 (see Fig. 6.1 (a))
126(3)
Diabatically avoided crossing case: β ≤ 0 (see Fig. 6.1(b))
129(6)
Other Exactly Solvable Models
135(10)
Two-State Problems
145(16)
Diagrammatic Technique
145(5)
Inelastic Scattering
150(1)
Elastic Scattering with Resonances and Predissociation
151(4)
Perturbed Bound States
155(3)
Time-Dependent Periodic Crossing Problems
158(3)
Effects of Dissipation and Fluctuation
161(8)
Multi-Channel Problems
169(30)
Exactly Solvable Models
169(7)
Time-independent case
169(2)
Time-dependent case
171(5)
Semiclassical Theory of Time-Independent Multi-Channel Problems
176(18)
General framework
179(1)
Case of no closed channel (m = 0)
180(1)
Case of m ≠ 0 at energies higher than the bottom of the highest adiabatic potential
180(2)
Case of m ≠ 0 at energies lower than the bottom of the highest adiabatic potential
182(3)
Numerical example
185(9)
Time-Dependent Problems
194(5)
Multi-Dimensional Problems
199(34)
Classification of Surface Crossing
200(3)
Crossing seam
200(1)
Conical intersection
201(1)
Renner-Teller effect
202(1)
Reduction to One-Dimensional Multi-Channel Problem
203(25)
Linear Jahn-Teller problem
203(7)
Collinear chemical reaction
210(5)
Three-dimensional chemical reaction
215(13)
Semiclassical Propagation Method
228(5)
Complete Reflection and Bound States in the Continuum
233(24)
One NT-Type Crossing Case
233(7)
Diabatically Avoided Crossing (DAC) Case
240(8)
Two NT-Type Crossings Case
248(9)
At energies above the top of the barrier: (Eu, ∞)
248(1)
At energies between the barrier top and the higher crossing: (E+, Eu)
249(2)
At energies in between the two crossing regions: (E-, E+)
251(1)
At energies below the crossing points: (-∞, E-)
252(1)
Numerical examples
252(5)
New Mechanism of Molecular Switching
257(42)
Basic Idea
257(1)
One-Dimensional Model
258(23)
Transmission in a pure system
258(9)
Transmission in a system with impurities
267(10)
Molecular switching
277(4)
Two-dimensional model
281(9)
Two-dimensional constriction model
282(3)
Wave functions, matching, and transmission coefficient
285(5)
Numerical Examples
290(9)
Control of Nonadiabatic Processes by an External Field
299(44)
Control of Nonadiabatic Transitions by Periodically Sweeping External Field
300(4)
Basic Theory
304(10)
Usage of the Landau-Zener-Stueckelberg type transition
310(2)
Usage of the Rosen-Zener-Demkov type transition
312(1)
General case
313(1)
Numerical Examples
314(15)
Spin tunneling by a magnetic field
314(2)
Vibrational and tunneling transitions by laser
316(3)
Landau-Zener-Stueckelberg type transition
319(4)
Rosen-Zener-Demkov type transition
323(1)
General case
324(5)
Laser Control of Photodissociation with Use of the Complete Reflection Phenomenon
329(14)
Conclusions: Future Perspectives
343(4)
Appendix A Final Recommended Formulas for General Time-Independent Two-Channel Problem 347(12)
A.1. Landau-Zener Type
347(5)
A.1.1. E ≥ Ex (crossing energy) (b2 ≥ 0)
349(1)
A.1.2. E ≤ Ex (b2 ≤ 0)
350(1)
A.1.3. Total scattering matrix
351(1)
A.2. Nonadiabatic Tunneling Type (see Fig. A.2)
352(7)
A.2.1 E ≥ Eb
355(1)
A.2.2. Eb ≥ E ≥ Et
355(2)
A.2.3. E ≤ Et
357(2)
Appendix B Time-Dependent Version of the Zhu-Nakamura Theory 359(2)
Bibliography 361(10)
Index 371

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